NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = P.R.Lornie Found 18 matches. 1979EK01 Nucl.Instrum.Methods 158, 243 (1979) L.P.Ekstrom, A.M.Al-Naser, P.R.G.Lornie, P.J.Twin Spin-Alignment Attenuation Factors in Mass 61-67 Nuclei Populated by (α, n) and (α, p) Reactions COMPILATION A=61-67; compiled, evaluated data on Iγ(θ) for E2 transitions observed in (α, n), (α, p); deduced spin-alignment attenuation factors α2, α4.
1979MO22 J.Phys.(London) G5, 1751 (1979) T.P.Morrison, G.D.Jones, L.P.Ekstrom, F.Kearns, A.Kogan, P.R.G.Lornie, O.Mustaffa, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth Coulomb-Nuclear Interference in the (7Li, 7Li) Reactions NUCLEAR REACTIONS 46,48Ti(7Li, 7Li'), E=17 MeV; 58Ni(7Li, 7Li'), E=19 MeV; measured σ(θ); deduced optical potentials. DWBA analyses.
doi: 10.1088/0305-4616/5/12/014
1978KO11 J.Phys.(London) G4, 755 (1978) A.Kogan, P.R.G.Lornie, G.D.Jones, M.R.Nixon, H.G.Price, R.Wadsworth, P.J.Twin Gamma-Ray Studies of the Odd-Parity States in Zn Isotopes. I. 65Zn NUCLEAR REACTIONS 62Ni(α, nγ), E=8.0-14.0 MeV; measured γγ-coin, γ(θ), linear polarization, DSA. 65Zn deduced levels, J, π, δ, T1/2, γ-branching. Enriched target, Ge(Li) detectors. Phonon-quasiparticle-coupling, shell-model calculations.
doi: 10.1088/0305-4616/4/5/010
1978LO06 J.Phys.(London) G4, 923 (1978) P.R.G.Lornie, A.Kogan, G.D.Jones, M.R.Nixon, H.G.Price, R.Wadsworth, P.J.Twin Gamma-Ray Studies of the Odd-Parity States in Zn Isotopes. II. Levels Below 2.0 MeV in Excitation Energy in 67Zn NUCLEAR REACTIONS 64Ni(α, nγ), E=6.5-17.0 MeV; measured γγ-coin, γ(θ), linear polarization, DSA. 67Zn deduced levels, J, π, δ, T1/2, γ-branching. Enriched targets, Ge(Li) detectors.
doi: 10.1088/0305-4616/4/6/021
1978MU02 J.Phys.(London) G4, 99 (1978) O.M.Mustaffa, A.Kogan, G.D.Jones, P.R.G.Lornie, T.P.Morrison, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth Nuclear Spectroscopy in 63Zn: States below 1.5 MeV NUCLEAR REACTIONS 60Ni(α, nγ), E=8-16 MeV; measured Eγ, Iγ(E, θ), γγ-coin, linear polarization, DSA. 63Zn levels deduced T1/2, J, π, λ, δ, γ-branching. Enriched target, Ge(Li) detectors.
doi: 10.1088/0305-4616/4/1/011
1978PR02 J.Phys.(London) G4, 707 (1978) H.G.Price, G.D.Jones, P.R.G.Lornie, P.J.Twin, R.Wadsworth High Spin States in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=9.5, 16.0 MeV; measured σ(Eγ), polarization, Doppler shift. 42Ca levels deduced J, π, T1/2, δ.
doi: 10.1088/0305-4616/4/5/007
1978SI02 J.Phys.(London) G4, 111 (1978) D.N.Simister, G.D.Jones, A.Kogan, P.R.G.Lornie, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, R.Wadsworth Gamma Ray Spectroscopy in 64Zn-Levels below 3.1 MeV in Excitation NUCLEAR REACTIONS 61Ni(α, nγ), E=7.8 MeV; measured Eγ, Iγ(θ), linear polarization, DSA. 64Zn deduced levels, J, π, T1/2, λ, δ. Enriched targets, Ge(Li) detectors.
doi: 10.1088/0305-4616/4/1/012
1978SI10 J.Phys.(London) G4, 1127 (1978) D.N.Simister, G.D.Jones, F.Kearns, A.Kogan, P.R.G.Lornie, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, R.Wadsworth Quasi-Band Structure in 64Zn NUCLEAR REACTIONS 61Ni(α, nγ), E=9.35 MeV; 56Fe(11B, 2npγ), E=30 MeV; measured γ(θ), DSA, linear polarization, σ(Eγ). 64Zn deduced levels, J, π, T1/2, γ-branching, B(λ). Enriched targets, Ge(Li) detectors. Shell model.
doi: 10.1088/0305-4616/4/7/017
1977LO03 J.Phys.(London) G3, 493 (1977) P.R.G.Lornie, A.Kogan, G.D.Jones, M.R.Nixon, H.G.Price, R.Wadsworth, P.J.Twin Further Evidence for Particle-Vibration Coupling among the Positive Parity States of 65,67Zn NUCLEAR REACTIONS 62,64Ni(α, nγ), E=6.5-17.0 MeV; measured σ(E, Eγ, θ), γγ-coin, linear polarization, DSA. 65,67Zn deduced levels, J, π, T1/2, δ, γ-branching, λ. Enriched targets, Ge(Li) detectors.
doi: 10.1088/0305-4616/3/4/011
1977WA03 J.Phys.(London) G3, 35 (1977) R.Wadsworth, A.Kogan, P.R.G.Lornie, M.R.Nixon, H.G.Price, P.J.Twin Gamma Ray Spectroscopy in 61Ni - Levels below 2.2 MeV in Excitation NUCLEAR REACTIONS 58Fe(α, nγ), E=6.5-13 MeV; measured σ(E, Eγ, θ), γγ-coin, linear polarization, DSA. 61Ni deduced levels, J, π, δ, γ-branching, T1/2. Enriched targets, Ge(Li) detectors. Shell model calculations.
doi: 10.1088/0305-4616/3/1/007
1977WA07 J.Phys.(London) G3, 833 (1977) R.Wadsworth, G.D.Jones, A.Kogan, P.R.G.Lornie, T.Morrison, O.Mustaffa, H.G.Price, D.Simister, P.J.Twin Gamma Ray Spectroscopy in 61Ni-Levels Above 2.2 MeV in Excitation NUCLEAR REACTIONS 53Cr(11B, 2npγ), E=30 MeV; 58Fe(α, nγ), E=6.5-13.0 MeV; measured γγ-coin, linear polarization, γ(θ), DSA. 61Ni deduced levels, J, π, T1/2, δ, γ-branching. Enriched targets, Ge(Li) detectors, shell-model calculations.
doi: 10.1088/0305-4616/3/6/014
1977WA15 J.Phys.(London) G3, 1377 (1977) R.Wadsworth, G.D.Jones, A.Kogan, P.R.G.Lornie, T.Morrison, O.Mustaffa, H.G.Price, D.N.Simister, P.J.Twin Lifetimes in 61Ni Measured by the Recoil Distance Technique NUCLEAR REACTIONS 58Fe(α, nγ), E=9.0 MeV; measured recoil distance. 61Ni levels deduced T1/2. Enriched targets, Ge(Li) detectors. Shell model comparison.
doi: 10.1088/0305-4616/3/10/012
1976PR15 J.Phys.(London) G2, L177 (1976) H.G.Price, G.D.Jones, P.R.G.Lornie, M.R.Nixon, P.J.Nolan, P.J.Twin Deformed Negative Parity States in 42Ca NUCLEAR REACTIONS 39K(α, pγ), E=9.5, 11.5 MeV; measured σ(Eγ), polarization, DSA, recoil distance. 42Ca levels deduced J, π, T1/2, δ. Separated isotope target.
doi: 10.1088/0305-4616/2/10/003
1975NA06 J.Phys.(London) G1, 324 (1975) A.Nagel, G.D.Jones, P.R.G.Lornie, M.R.Nixon, H.G.Price, P.J.Twin Further Evidence of Rotational Structure in 26Mg NUCLEAR REACTIONS 26Mg(α, α'γ), E=17.1 MeV; measured αγ-coin, γγ(θ). 26Mg levels deduced γ-mixing, γ-branching ratios, J.
doi: 10.1088/0305-4616/1/3/007
1975NI01 J.Phys.(London) G1, 430 (1975) M.R.Nixon, G.D.Jones, P.R.G.Lornie, A.Nagel, P.J.Nolan, H.G.Price, P.J.Twin High Spin Negative Parity States in 33P NUCLEAR REACTIONS 30Si(α, pγ), E=17 MeV; measured σ(Eγ, θ), γγ-coin, p, pγ(θ), recoil distance. 33P levels deduced J, π, γ-mixing, γ-branching.
doi: 10.1088/0305-4616/1/4/007
1974LO17 J.Phys.(London) A7, 1977 (1974) P.R.G.Lornie, E.M.Jayasinghe, G.D.Jones, H.G.Price, M.F.Thomas, P.J.Twin, P.J.Nolan High Spin Negative Parity States in 35Cl NUCLEAR REACTIONS 32S(α, pγ); measured pγ(θ), P(θ), DSA, recoil distance. 35Cl levels deduced J, π, γ-mixing, T1/2, γ-branching ratios, transition strengths.
doi: 10.1088/0305-4470/7/16/002
1974NA22 J.Phys.(London) A7, 1697 (1974) A.Nagel, G.D.Jones, P.R.G.Lornie, M.R.Nixon, H.G.Price, P.J.Twin Rotational States in 26Mg NUCLEAR REACTIONS 26Mg(p, p'γ), E=7.6 MeV; measured p'γ-coin, p'γ(θ). 23Na(α, pγ), E=7.3 MeV; measured DSA. 26Mg(α, α'γ), E=16.97-17.1 MeV; measured α'γ-coin, Iγ(θ). 26Mg levels deduced T1/2, mixing ratios, J, π.
doi: 10.1088/0305-4470/7/14/002
1974TW01 J.Phys.(London) A7, 1410 (1974) P.J.Twin, E.M.Jayasinghe, G.D.Jones, P.R.G.Lornie, A.Nagel, H.G.Price, M.F.Thomas Gamma-Ray Spectroscopy in 31P: Levels below 7-5 MeV NUCLEAR REACTIONS 28Si(α, pγ), E=17 MeV; measured Eγ, Iγ, pγ-coin, DSA, pγ, γ(θ), pγ(θ). 31P deduced levels, J, π, γ-mixing, γ-branching ratios, T1/2.
doi: 10.1088/0305-4470/7/12/005
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